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All results from a given calculation for C2H4O2 (1,3-dioxetane)

using model chemistry: B1B95/cc-pVDZ

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 yes D2H 1Ag
Energy calculated at B1B95/cc-pVDZ
 hartrees
Energy at 0K-228.931504
Energy at 298.15K-228.937211
Nuclear repulsion energy131.450598
The energy at 298.15K was derived from the energy at 0K and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/cc-pVDZ
Mode Number Symmetry Frequency
(cm-1)
Scaled Frequency
(cm-1)
IR Intensities
(km mol-1)
Raman Act
4/u)
Dep P Dep U
1 Ag 3017 2900 0.00      
2 Ag 1563 1503 0.00      
3 Ag 1157 1112 0.00      
4 Ag 902 867 0.00      
5 Au 1124 1080 0.00      
6 B1g 1331 1279 0.00      
7 B1g 1060 1019 0.00      
8 B1u 3056 2938 171.78      
9 B1u 1167 1122 18.63      
10 B1u 157 151 11.75      
11 B2g 3052 2934 0.00      
12 B2g 1121 1078 0.00      
13 B2u 1447 1390 27.39      
14 B2u 994 956 101.32      
15 B3g 1057 1016 0.00      
16 B3u 2997 2881 235.24      
17 B3u 1524 1465 21.34      
18 B3u 1126 1083 259.81      

Unscaled Zero Point Vibrational Energy (zpe) 13925.9 cm-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 13385.5 cm-1
See section III.C.1 List or set vibrational scaling factors to change the scale factors used here.
See section III.C.2 Calculate a vibrational scaling factor for a given set of molecules to determine the least squares best scaling factor.
Rotational Constants (cm-1) from geometry optimized at B1B95/cc-pVDZ
ABC
0.46383 0.45351 0.25199

See section I.F.4 to change rotational constant units
Geometric Data calculated at B1B95/cc-pVDZ

Point Group is D2h

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
C1 -0.972 0.000 0.000
C2 0.972 0.000 0.000
O3 0.000 1.029 0.000
O4 0.000 -1.029 0.000
H5 -1.605 0.000 0.906
H6 1.605 0.000 0.906
H7 -1.605 0.000 -0.906
H8 1.605 0.000 -0.906

Atom - Atom Distances (Å)
  C1 C2 O3 O4 H5 H6 H7 H8
C11.94311.41511.41511.10532.73091.10532.7309
C21.94311.41511.41512.73091.10532.73091.1053
O31.41511.41512.05772.11052.11052.11052.1105
O41.41511.41512.05772.11052.11052.11052.1105
H51.10532.73092.11052.11053.20941.81203.6856
H62.73091.10532.11052.11053.20943.68561.8120
H71.10532.73092.11052.11051.81203.68563.2094
H82.73091.10532.11052.11053.68561.81203.2094

picture of 1,3-dioxetane state 1 conformation 1
More geometry information
Calculated Bond Angles
atom1 atom2 atom3 angle atom1 atom2 atom3 angle
C1 O3 C2 86.719 C1 O4 C2 86.719
O3 C1 O4 93.281 O3 C1 H5 113.159
O3 C1 H7 113.159 O3 C2 O4 93.281
O3 C2 H6 113.159 O3 C2 H8 113.159
O4 C1 H5 113.159 O4 C1 H7 113.159
O4 C2 H6 113.159 O4 C2 H8 113.159
H5 C1 H7 110.105 H6 C2 H8 110.105
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ Charges (e)
Number Element Mulliken CHELPG AIM ESP
1 C 0.267      
2 C 0.267      
3 O -0.335      
4 O -0.335      
5 H 0.034      
6 H 0.034      
7 H 0.034      
8 H 0.034      


Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section VII.A.3)
  x y z Total
  0.000 0.000 0.000 0.000
CHELPG        
AIM        
ESP        


Electric Quadrupole moment
Quadrupole components in D Å
Primitive
 xyz
x -18.900 0.000 0.000
y 0.000 -27.933 0.000
z 0.000 0.000 -22.562
Traceless
 xyz
x 6.347 0.000 0.000
y 0.000 -7.202 0.000
z 0.000 0.000 0.855
Polar
3z2-r21.709
x2-y29.032
xy0.000
xz0.000
yz0.000


Polarizabilities
Components of the polarizability tensor.
Units are Å3 (Angstrom cubed)
Change units.
  x y z
x 5.150 0.000 0.000
y 0.000 2.985 0.000
z 0.000 0.000 3.661


<r2> (average value of r2) Å2
<r2> 56.295
(<r2>)1/2 7.503